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Minimal Models of Adapted Neuronal Response to In Vivo–Like ...

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Adapting Rate <strong>Models</strong> 2103<br />

We show that under such conditions, Ermentrout’s model can be easily<br />

generalized, and the adapted response can be obtained as the fixed point <strong>of</strong><br />

f = (m − αf, s). For this result <strong>to</strong> hold, it is necessary that adaptation is<br />

slow compared <strong>to</strong> the timescale <strong>of</strong> the neural dynamics. <strong>In</strong> such a case, the<br />

feedback current αf is a slowly fluctuating variable and does not affect the<br />

value <strong>of</strong> s. Note that a slow adaptation is a minimal request in the absence<br />

<strong>of</strong> noise (Ermentrout, 1998).<br />

The proposed model is very general, but it can be used <strong>to</strong> full advantage<br />

only if the response function is known analytically. This is the case <strong>of</strong> simple<br />

model neurons, for which the rate function can be calculated, or more<br />

complex neurons whose f-I curve can be fitted by a suitable model function<br />

(e.g., Larkum, Senn, & Lüscher, in press). <strong>In</strong> section 2, the adapting rate<br />

model is introduced and tested on several versions <strong>of</strong> IF neurons, whose<br />

rate functions are known and easily computable. The resulting rate models<br />

are checked against the simulations <strong>of</strong> the full models from which they<br />

are derived, including the leaky IF (LIF) neuron with conductance-based<br />

synaptic inputs. Only slight variations are needed if a different mechanism<br />

<strong>of</strong> adaptation is considered, as, for example, an adapting threshold for spike<br />

emission, which is dealt with in section 2.2. Evidence is also provided that<br />

the LIF neuron with an adapting threshold is able <strong>to</strong> fit the response functions<br />

<strong>of</strong> rat pyramidal neurons (see section 2.3), a result that parallels those<br />

<strong>of</strong> Rauch et al. (2003) obtained with an afterhyperpolarization current. Finally,<br />

in section 3, we show how the stationary response function can be<br />

used <strong>to</strong> predict the time-varying activity <strong>of</strong> a large population <strong>of</strong> adapting<br />

neurons.<br />

2 Adapting Rate <strong>Models</strong> in the Presence <strong>of</strong> Noise<br />

Firing-rate adaptation is a complex phenomenon characterized by several<br />

timescales and affected by different ion currents. At least three phases <strong>of</strong><br />

adaptation have been documented in many in vitro preparations, referred <strong>to</strong><br />

as initial or one-interspike (ISI) interval adaptation, which affects the first or<br />

at most the first two ISIs (Schwindt, O’Brien, & Crill, 1997), early adaptation,<br />

involving the first few seconds, and late adaptation, shown in response <strong>to</strong> a<br />

prolonged stimulation (see Table 1 <strong>of</strong> Sawczuk, Powers, & Binder, 1997, for<br />

references and a list <strong>of</strong> possible mechanisms).<br />

<strong>In</strong>itial adaptation depends largely on Ca 2+ -dependent K + current (Sah,<br />

1996; Powers et al., 1999), although other mechanisms may also play a role<br />

(Sawczuk et al., 1997). The early and late phases <strong>of</strong> adaptation are not well<br />

unders<strong>to</strong>od, and several mechanisms have been put forward: in neocortical<br />

neurons, it seems that Na + -dependent K + currents (Schwindt, Spain, & Crill,<br />

1989; Sanchez-Vives, Nowak, & McCormick, 2000), and slow inactivation<br />

<strong>of</strong> Na + channels (Fleidervish, Friedman, & Gutnik, 1996) may play a major<br />

role; in mo<strong>to</strong>neurons, evidence is accumulating for an interplay between<br />

slow inactivation <strong>of</strong> Na + channels, which tend <strong>to</strong> decrease the firing rate,

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